CN1894781B - Method for fabricating a nitrided silicon-oxide gate dielectric - Google Patents
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Abstract
Description
技术领域technical field
本发明涉及半导体器件的制造;更具体地说,它涉及制造氮化氧化硅栅极介质的方法。The present invention relates to the fabrication of semiconductor devices; more particularly, it relates to methods of fabricating nitrided silicon oxide gate dielectrics.
背景技术Background technique
集成电路趋向较高性能、较高速度和较低成本。相应地,要缩小器件的维度和元件的尺寸,并且必须相应地按比例缩放栅极介质。当栅极介质物理厚度减小时,出现了对较高介电常数和较低泄漏栅极介质的需求。在先进金属氧化物半导体场效应晶体管(MOSFET)中,用氧氮化硅(SiOxNy)层作栅极介质。MOSFET晶体管包括在硅衬底中形成的沟道区域,在薄栅极介质层顶上形成并在沟道区域上对准的N或P掺杂多晶硅栅极,以及在沟道区域的任意一侧上的硅衬底中形成的源极/漏极区域。Integrated circuits are trending towards higher performance, higher speed and lower cost. Accordingly, device dimensions and component sizes are reduced, and the gate dielectric must be scaled accordingly. As the physical thickness of the gate dielectric decreases, the need for higher dielectric constant and lower leakage gate dielectrics arises. In advanced metal oxide semiconductor field effect transistors (MOSFETs), a silicon oxynitride (SiO x N y ) layer is used as the gate dielectric. A MOSFET transistor consists of a channel region formed in a silicon substrate, an N- or P-doped polysilicon gate formed atop a thin gate dielectric layer and aligned over the channel region, and on either side of the channel region source/drain regions formed on the silicon substrate.
然而,SiOxNy栅极介质的一个问题是经过晶片厚度和氮浓度的改变。栅极介质的经过晶片厚度和氮浓度的改变直接导致经过晶片阈值电压的改变,特别地,在P-沟道场效应晶体管(PFET)中,引起来自相同晶片的各个分离集成电路芯片的性能的改变。因此,需要一种制造具有相对均匀的经过晶片厚度和氮浓度的SiOxNy层的方法。However, one problem with SiOxNy gate dielectrics is through wafer thickness and nitrogen concentration changes . Variations in gate dielectric across-wafer thickness and nitrogen concentration directly result in changes in across-wafer threshold voltage and, in particular, in P-channel field-effect transistors (PFETs), cause changes in the performance of individual integrated circuit chips from the same wafer . Therefore, there is a need for a method of fabricating SiOxNy layers with relatively uniform across-wafer thickness and nitrogen concentration.
发明内容Contents of the invention
本发明的第一方面是一种制造栅极介质层的方法,包括以下步骤:提供衬底;在所述衬底的上表面上形成二氧化硅层;在还原气氛中执行等离子体氮化以将所述二氧化硅层转变为氧氮化硅层。A first aspect of the present invention is a method of manufacturing a gate dielectric layer, comprising the steps of: providing a substrate; forming a silicon dioxide layer on the upper surface of the substrate; performing plasma nitridation in a reducing atmosphere to The silicon dioxide layer is converted to a silicon oxynitride layer.
本发明的第二方面是一种制造MOSFET的方法,包括以下步骤:提供具有至少最上硅层的半导体衬底;在所述半导体衬底的上表面上形成二氧化硅层;在还原气氛中执行等离子体氮化以将所述二氧化硅层转变为氧氮化硅层;在所述氧氮化硅层上形成多晶硅栅极,所述多晶硅栅极在所述半导体衬底中的沟道区域上对准;以及在所述半导体衬底中形成源极/漏极区域,所述源极/漏极区域与所述多晶硅栅极对准。A second aspect of the present invention is a method of manufacturing a MOSFET comprising the steps of: providing a semiconductor substrate having at least an uppermost silicon layer; forming a silicon dioxide layer on the upper surface of said semiconductor substrate; performing in a reducing atmosphere plasma nitridation to convert the silicon dioxide layer into a silicon oxynitride layer; forming a polysilicon gate on the silicon oxynitride layer, the polysilicon gate in a channel region in the semiconductor substrate aligning above; and forming source/drain regions in the semiconductor substrate, the source/drain regions being aligned with the polysilicon gate.
附图说明Description of drawings
在附加权利要求中阐明了本发明的特征。然而,通过参考后面示意性实施例的详细描述并与附图一起阅读将会更好地理解发明本身,其中:The features of the invention are set forth in the appended claims. However, the invention itself will be better understood by reference to the following detailed description of illustrative embodiments read in conjunction with the accompanying drawings, in which:
图1至3是部分截面图,示出了根据本发明制造氮化栅极介质层;1 to 3 are partial cross-sectional views showing the fabrication of a nitrided gate dielectric layer according to the present invention;
图4和5是部分截面图,示出了根据本发明制造MOSFET;4 and 5 are partial cross-sectional views illustrating the fabrication of MOSFETs in accordance with the present invention;
图6是根据本发明用于制造在图1至4中示出的介质层和MOSFET的工艺步骤的流程图;Figure 6 is a flow chart of the process steps for fabricating the dielectric layer and MOSFET shown in Figures 1 to 4 in accordance with the present invention;
图7是根据本发明的第一实施例用于执行氮化步骤的远程等离子体系统氮化系统的示意图;7 is a schematic diagram of a remote plasma system nitridation system for performing a nitridation step according to a first embodiment of the present invention;
图8是根据本发明氮化氧化硅栅极介质的经过晶片厚度的控制改善的图表;Fig. 8 is a chart showing the improvement of wafer thickness control of silicon nitride oxide gate dielectric according to the present invention;
图9是根据本发明使用和不使用还原气体,氮化二氧化硅厚度的不同的图表;以及Figure 9 is a graph of the thickness of nitrided silicon dioxide with and without reducing gas according to the present invention; and
图10是根据本发明的第二实施例用于执行氮化步骤的远程等离子体系统氮化系统的示意图。10 is a schematic diagram of a remote plasma system nitridation system for performing a nitridation step according to a second embodiment of the present invention.
具体实施方式Detailed ways
术语氮化二氧化硅指向SiO2层中引入氮以形成氧氮化硅(SiOxNy)。SiOxNy的范围包括所有整数x和y(或其分数)的组合,其中SiOxNy是稳定的。还原气氛限定为包括与氧反应的核素的气态气氛。The term silicon dioxide nitride refers to the introduction of nitrogen into the SiO2 layer to form silicon oxynitride ( SiOxNy ). The range of SiO x N y includes all combinations of integers x and y (or fractions thereof) in which SiO x N y is stable. A reducing atmosphere is defined as a gaseous atmosphere that includes nuclides that react with oxygen.
图1至3是部分截面图,示出了根据本发明制造氮化物栅极介质层。在图1中,提供具有上表面105的衬底100。衬底100可以是本征、N-型或P-型体硅衬底,未掺杂或本征、N-型或P-型绝缘体上硅(SOI)衬底或蓝宝石衬底或红宝石衬底。1 to 3 are partial cross-sectional views illustrating the fabrication of a nitride gate dielectric layer according to the present invention. In FIG. 1 , a
在图2中,在衬底100的上表面105上形成具有厚度D1的基体SiO2层110。在表面105上形成基体SiO2层110之前,通过技术上已公知的多个清洁工艺的任意一个清洁该表面。例如,可以使用稀释氢氟酸(BHF)清洁之后NH4OH清洁再之后HCl清洁来清洁表面105。如果衬底100是块体硅衬底或SOI衬底,可以在第一实例中,通过在含氧气氛的炉中,在约600到800℃温度下热氧化约0.5到30分钟,形成基体SiO2层110。在第二实例中,可以通过在含氧气氛中,在约800到1000℃温度下快速热氧化(RTO)约5到60秒,形成基体SiO2层110。如果衬底100是红宝石或蓝宝石衬底,可以通过在化学气相沉积(CVD)装置中沉积形成基体SiO2层110并且介质层可以是四乙氧基硅烷(TEOS)氧化物。TEOS还可以用于体硅或SOI衬底。TEOS还可以用于体硅或SOI衬底。在一个实例中,D1约8到厚。对任意衬底,基体SiO2层110可以是自然氧化物,允许通过将清洁硅表面暴露在空气或氧气中形成,或基体SiO2层110可以通过“裸”硅表面的氧化清洁工艺形成。In FIG. 2 , a base SiO 2 layer 110 having a thickness D1 is formed on the
在图3中,执行远程等离子体氮化(RPN)工艺以将基体SiO2层110(见图2)转变为氮化SiO2(SiOxNy)层110A。下面参考图6,7和9描述远程等离子体氮化工艺。SiOxNy层110A具有厚度D2。在一个实例中,D2约8到厚。在一个实例中,SiOxNy层110A约2到20%的氮原子。在第二实例中,在SiOxNy层110A中的氮的浓度在1E21和1E22atm/cm3之间。本发明的一个优点是氮化后氧化物的介质厚度与氮化前氧化物的厚度相比增加很小。尽管厚度增加的数量是氮化前氧化物的厚度(D1)的函数,氮化后氧化物的厚度(D2)通常仅增加约0到5%。In FIG. 3 , a remote plasma nitriding (RPN) process is performed to transform the base SiO 2 layer 110 (see FIG. 2 ) into a nitrided SiO 2 (SiO x N y )
图4和5是部分截面图,示出了根据本发明制造MOSFET。图4延续图3。在图4中,在SiOxNy层110A的上表面上形成多晶硅层115。可以使用技术上已公知的如低压化学气相沉积(LPCVD)或快速热化学气相沉积(RTCVD)的许多沉积工艺的一种形成多晶硅层115。多晶硅层115可以是未掺杂或掺杂N-型或P-型。在一个实例中,多晶硅层115是1000到厚。4 and 5 are partial cross-sectional views showing the fabrication of MOSFETs according to the present invention. FIG. 4 is a continuation of FIG. 3 . In FIG. 4, a
在图5中,蚀刻多晶硅层115(参看图4);例如,通过反应离子蚀刻(RIE)工艺以形成栅极125。在栅极125的侧壁135上形成隔离物130。源极/漏极140的形成(典型地通过一步或多步离子注入工艺)基本上完成MOSFET 145的形成,SiOxNy层110A作为MOSFET的栅极介质.如果多晶硅层115(参看图4)在沉积期间未掺杂,形成隔离物后,栅极125可以与源极/漏极140的形成一起或通过分离步骤,通过离子注入掺杂N-型或P-型.In FIG. 5 , polysilicon layer 115 (see FIG. 4 ) is etched; for example, by a reactive ion etching (RIE) process to form gate 125 . Spacers 130 are formed on sidewalls 135 of gate 125 . The formation of the source/drain 140 (typically by one or more steps of ion implantation process) basically completes the formation of the MOSFET 145, and the SiO x N y layer 110A acts as the gate dielectric of the MOSFET. If the polysilicon layer 115 (see FIG. 4) Undoped during deposition, after formation of spacers, gate 125 can be doped N-type or P-type by ion implantation together with the formation of source/drain 140 or through a separate step.
图6是根据本发明,在图1至5中示出的用于形成介质层和MOSFET的工艺步骤的流程图。将以硅衬底为例。在步骤150中,通过技术上已公知的多个清洁工艺的任意一个清洁硅衬底的表面。在第一实例中,可以使用稀释氢氟酸(BHF)清洁之后NH4OH清洁再之后HCl清洁,来清洁硅表面105。可选地,在第二实例中,可以使用BHF之后O3清洁再之后干HCl清洁,来清洁硅表面。FIG. 6 is a flow chart of the process steps shown in FIGS. 1 to 5 for forming the dielectric layer and MOSFET in accordance with the present invention. A silicon substrate will be taken as an example. In
在步骤155中,例如,通过在含氧气氛的炉中,在约600到800℃温度下热氧化约0.5到30分钟,通过在含氧气氛中,在约800到1000℃温度下RTO约5到60秒,或通过将清洁硅表面暴露于空气或氧气,来形成基体SiO2层。基体SiO2层约8到厚。In step 155, for example, by thermal oxidation at a temperature of about 600 to 800° C. in an oxygen-containing atmosphere for about 0.5 to 30 minutes, by RTO of about 5 at a temperature of about 800 to 1000° C. in an oxygen-containing atmosphere to 60 s, or by exposing the cleaned silicon surface to air or oxygen, to form a base SiO2 layer. The base SiO 2 layer is about 8 to thick.
在步骤160中,执行远程等离子体氮化工艺。在第一实例中,将氮和如氦的惰性气体的混合气体引入远程等离子体氮化装置的等离子体产生端口,并将如氢或氨的还原气体通过第二、非等离子体产生端口引入,同时在处理反应室中旋转将要处理的晶片(参看图7)。典型的工艺条件是氮的流速约1到20slm(标准升/分),氦(或其它惰性气体)的流速约1到20slm,氢(氨或其它还原气体)的流速约1到20slm,反应室气压约0.2到50Torr,微波功率1000到3000瓦特,晶片温度约25到1000℃,持续约20到500秒。In step 160, a remote plasma nitridation process is performed. In a first example, a mixture of nitrogen and an inert gas such as helium is introduced into a plasma generating port of a remote plasma nitriding apparatus and a reducing gas such as hydrogen or ammonia is introduced through a second, non-plasma generating port, Simultaneously, the wafer to be processed is rotated in the processing chamber (see FIG. 7). Typical process conditions are that the flow rate of nitrogen is about 1 to 20 slm (standard liter/minute), the flow rate of helium (or other inert gas) is about 1 to 20 slm, and the flow rate of hydrogen (ammonia or other reducing gas) is about 1 to 20 slm. The air pressure is about 0.2 to 50 Torr, the microwave power is 1000 to 3000 watts, the wafer temperature is about 25 to 1000° C., and the duration is about 20 to 500 seconds.
在第二实例中,将氮、如氦的惰性气体和如氢或氨的还原气体的混合气体引入远程等离子体氮化装置的等离子体产生端口,同时在处理反应室中旋转将要处理的晶片(参看图10)。典型的工艺条件是氮的流速约1到20slm,氦(或其它惰性气体)的流速约1到20slm,氢的流速约1到20slm,反应室气压约0.2到50Torr,微波功率1000到3000瓦特,晶片温度约25到1000℃,持续约20到500秒。In the second example, a mixed gas of nitrogen, an inert gas such as helium, and a reducing gas such as hydrogen or ammonia is introduced into a plasma generation port of a remote plasma nitridation apparatus while rotating a wafer to be processed in a processing chamber ( See Figure 10). Typical process conditions are that the flow rate of nitrogen is about 1 to 20 slm, the flow rate of helium (or other inert gas) is about 1 to 20 slm, the flow rate of hydrogen is about 1 to 20 slm, the reaction chamber pressure is about 0.2 to 50 Torr, and the microwave power is 1000 to 3000 watts, The wafer temperature is about 25 to 1000° C. for about 20 to 500 seconds.
在这两个实例中,氮的剂量约1E14到5E15atm/cm2并且最终SiOxNy层含有约2到20%的氮。In both examples , the dose of nitrogen was about 1E14 to 5E15 atm/cm 2 and the final SiOxNy layer contained about 2 to 20% nitrogen.
在步骤165中,执行可选的退火步骤。通常不需要退火,因为在热晶片上实施远程等离子体氮化。可以执行标准的快速热退火(RTA)或峰值RTA。使用峰值退火以提高迁移率而不驱使氮进入SiO2/Si界面。峰值退火限定为晶片在最高晶片温度的时间约60秒或更短的退火,而标准RTA限定为晶片在最高晶片温度的时间大于约60秒的退火。In
之后的步骤使用氮化SiO2介质作为MOSFET的栅极介质。Later steps use a nitrided SiO2 dielectric as the gate dielectric for the MOSFET.
在步骤170中,使用技术上已公知的如LPCVD或RTCVD的多种沉积工艺的一种在氮化SiO2上形成多晶硅层。该多晶硅层可以未掺杂或掺杂N-型或P-型。在一个实例中,多晶硅层是1000到厚。In
在步骤175中,基本上完成了MOSFET。蚀刻多晶硅层;例如,通过RIE工艺形成栅极,在栅极的侧壁上形成隔离物并且在栅极的任意一侧上的衬底中形成源极/漏极(典型地通过一步或多步离子注入工艺)。SiOxNy层是MOSFET的栅极介质。如果多晶硅层在沉积期间未掺杂,形成隔离物后,栅极可以与源极/漏极140的形成一起或通过分离的步骤,通过离子注入掺杂N-型或P-型。In
图7是根据本发明的第一实施例,用于执行氮化步骤的远程等离子体系统氮化系统的示意图.在图7中,远程等离子体装置180包括反应室185和在反应室中的可旋转晶片卡盘190(用于夹持晶片195).用于提供能量以启动并维持等离子体205的微波线圈200包围反应室185的内壁215中的第一入口210A.通过入口210A提供用于产生等离子体205的气体(在本实例中,氦/氮混合气体).通过第二入口210B提供还原气体(在本实例中,氢).其它还原气体包括氨,氢和氮的混合气体,氨和氮的混合气体,以及氢、氨和氮的混合气体,氘,氘化氨,氘和氮的混合气体,氘化氨和氮的混合气体,氘、氘化氨和氮的混合气体,以及氘、氨和氮的混合气体.也在反应室185的内壁215中并与真空泵(未示出)相连的排气口220移除废核素并维持处理气压.排气口220和第一入口210A位于室185的直径相对侧,并且第二入口210B位于第一入口和排气口之间.Figure 7 is a schematic diagram of a remote plasma system nitriding system for performing a nitriding step according to a first embodiment of the present invention. In Figure 7, a remote plasma device 180 includes a reaction chamber 185 and possible Rotating wafer chuck 190 (for holding wafer 195). Microwave coil 200 for providing energy to start and maintain plasma 205 surrounds first inlet 210A in inner wall 215 of reaction chamber 185. Provides for generating The gas of the plasma 205 (in this example, a helium/nitrogen mixed gas). A reducing gas (in this example, hydrogen) is provided through the second inlet 210B. Other reducing gases include ammonia, a mixture of hydrogen and nitrogen, ammonia and Mixed gases of nitrogen, mixed gases of hydrogen, ammonia and nitrogen, deuterium, deuterated ammonia, mixed gases of deuterium and nitrogen, mixed gases of deuterated ammonia and nitrogen, mixed gases of deuterium, deuterated ammonia and nitrogen, and deuterium , a mixed gas of ammonia and nitrogen. Also in the inner wall 215 of the reaction chamber 185 and connected to the vacuum pump (not shown), the exhaust port 220 removes spent nuclides and maintains the process gas pressure. The exhaust port 220 and the first inlet 210A Located on the diametrically opposite side of chamber 185, and the second inlet 210B is located between the first inlet and the exhaust port.
使用中,具有在晶片230上表面上的基体SiO2层(未示出)的晶片195从转换反应室(未示出)放入反应室185中并且旋转,通过第一入口210A将预定氮化气体混合物(在本实例中,He/N2)以预定流速引入反应室,通过第二入口B将预定还原气体混合物(在本实例中,H2/NH3)以预定流速引入反应室,并且反应室通过与排气口220相连的真空泵维持预定气压。将预定瓦特数的微波功率施加到微波线圈200上,以激励并维持等离子体205。在预定时间后,断开微波功率熄灭等离子体205,切断气流并且反应室185的气压达到转换反应室的气压。等离子体205主要是氮离子、氦离子、氢中性等离子体。In use, a wafer 195 having a matrix SiO2 layer (not shown) on the upper surface of the wafer 230 is placed into the reaction chamber 185 from a conversion reaction chamber (not shown) and rotated, a predetermined nitridation process is carried out through the first inlet 210A. a gas mixture (in this example, He/N 2 ) is introduced into the reaction chamber at a predetermined flow rate, a predetermined reducing gas mixture (in this example, H 2 /NH 3 ) is introduced into the reaction chamber at a predetermined flow rate through the second inlet B, and The reaction chamber is maintained at a predetermined pressure by a vacuum pump connected to the exhaust port 220 . A predetermined wattage of microwave power is applied to microwave coil 200 to energize and maintain plasma 205 . After a predetermined time, the microwave power is turned off to extinguish the plasma 205, the gas flow is shut off and the pressure of the reaction chamber 185 reaches the pressure of the conversion reaction chamber. The plasma 205 is mainly nitrogen ion, helium ion, hydrogen neutral plasma.
用于实践本发明的合适装置的一个实例是由Applied Materials Corp,Santa Clara,CA制造的AMAT model XE12反应室,具有也是由AppliedMaterials Corp提供的解耦等离子体单元。An example of a suitable apparatus for practicing the invention is an AMAT model XE12 reaction chamber manufactured by Applied Materials Corp, Santa Clara, CA, with a decoupled plasma cell also supplied by Applied Materials Corp.
图8是根据本发明氮化氧化硅栅极介质的经过晶片厚度的控制改善的图表。图8示出了对于平均厚度相同的两个氮化二氧化硅膜,RPN后氧化硅膜的厚度对与晶片中心的距离的函数。使用椭偏仪执行测量。曲线225是如上述处理的SiOxNy层,但是没有任何还原气体流。曲线225的SiOxNy层的平均厚度是具有0.97的δ。曲线230是如上述处理的SiOxNy层,但是具有还原气体流。曲线230的SiOxNy层的平均厚度是具有0.50的δ。因此,引入还原核素导致厚度不均匀的约双倍的增加。FIG. 8 is a graph showing the improvement in control over wafer thickness for a silicon nitride oxide gate dielectric in accordance with the present invention. Figure 8 shows the thickness of the silicon oxide film after RPN as a function of the distance from the center of the wafer for two silicon dioxide nitride films of the same average thickness. Measurements are performed using an ellipsometer. Curve 225 is the SiOxNy layer treated as above, but without any reducing gas flow. The average thickness of the SiO x N y layer of curve 225 is Has a delta of 0.97. Curve 230 is the SiOxNy layer treated as above, but with reducing gas flow. The average thickness of the SiO x N y layer of curve 230 is Has a delta of 0.50. Thus, the introduction of reducing nuclides results in approximately a two-fold increase in thickness non-uniformity.
层225和230的第二离子质谱分析(SIMS)分布说明氮浓度均匀性的提高与SiOxNy厚度均匀性的提高轨迹复合很好,如表I所示。注意氮的剂量和浓度之间是一一对应的。The second ion mass spectrometry (SIMS) profiles of layers 225 and 230 show that the increase in nitrogen concentration uniformity compounded well with the increase in SiOxNy thickness uniformity , as shown in Table I. Note that there is a one-to-one correspondence between nitrogen dose and concentration.
表ITable I
在表I中,在没有还原气体存在的反应室中,由远程等离子体氮化处理的晶片中,氮浓度从中心到边缘的改变超过50%。在具有还原气体存在的反应室中,由远程等离子体氮化处理的晶片的两个实例中,在晶片中氮浓度从中心到边缘的改变不超过25%。In Table I, the nitrogen concentration varies by more than 50% from the center to the edge in wafers treated by remote plasma nitridation in a chamber in which no reducing gas is present. In both instances of wafers treated by remote plasma nitridation in a reaction chamber with a reducing gas present, the nitrogen concentration in the wafer did not vary by more than 25% from the center to the edge.
因此,SiOxNy厚度的均匀性和氮浓度的均匀性都有约两倍因子的提高。Consequently, both the SiOxNy thickness uniformity and the nitrogen concentration uniformity are improved by a factor of about two.
图9是根据本发明使用和不使用还原气体,氮化二氧化硅厚度的不同的图表.如上所述,在执行RPN处理时不使用还原气体的另一个问题是,如所示的在基体SiO2层和完成的SiOxNy层之间介质厚度有不可接受的增加。如图9所示,向RPN反应室中引入还原气体大大降低了此厚度的增加。图9绘出了自然氧化(曲线235)、RPN后自然氧化膜无还原气体处理(曲线240)和RPN后自然氧化膜有还原气体处理(曲线245)的厚度对与晶片中心的距离的函数。使用椭偏仪执行测量。曲线240是SiOxNy层,由约厚的自然氧化层经上述处理制备,但是没有任何还原气体流。曲线240的SiOxNy层的平均厚度约25到曲线245是如上述处理的SiOxNy层,但是具有还原气体流。曲线245的平均厚度约13到因此,引入还原核素明显减小了介质层厚度在RPN处理期间的增加。厚度的增加限定在约35%。在一些实例中厚度的增加接近于零。Figure 9 is a graph of the thickness of nitrided silicon dioxide with and without the use of a reducing gas according to the present invention. As mentioned above, another problem with performing the RPN process without using a reducing gas is that, as shown in the substrate SiO There is an unacceptable increase in dielectric thickness between layer 2 and the finished SiO x N y layer. As shown in Figure 9, the introduction of reducing gas into the RPN reaction chamber greatly reduced this thickness increase. 9 plots the thickness of native oxidation (curve 235), post-RPN native oxide film without reducing gas treatment (curve 240), and post-RPN native oxide film with reducing gas treatment (curve 245) as a function of distance from the wafer center. Measurements are performed using an ellipsometer.
图10是根据本发明的第二实施例用于执行氮化步骤的远程等离子体系统氮化系统的示意图。图10类似于图7,除了没有气体从第二入口210B提供而所有的气体(氮,氦和氢)都通过第一入口210A提供。等离子体205主要是氮离子、氦离子、氢离子等离子体。10 is a schematic diagram of a remote plasma system nitridation system for performing a nitridation step according to a second embodiment of the present invention. Figure 10 is similar to Figure 7 except that no gas is provided from the second inlet 210B and all gases (nitrogen, helium and hydrogen) are provided through the first inlet 210A. The plasma 205 is mainly nitrogen ion, helium ion, hydrogen ion plasma.
因此,本发明满足了对具有相对均匀的经过晶片厚度的SiOxNy层的制造方法的需求。Thus , the present invention fulfills the need for a method of fabricating a SiOxNy layer with a relatively uniform thickness across the wafer.
上面给出的本发明的实施例的描述用于理解本发明。应该明白,本发明不仅仅限于这里描述的特殊的实施例,而是现在对于本领域的技术人员明白的是,在不脱离本发明的范围内可以进行各种修改,重新布置以及替代。因此,旨在随后的权利要求覆盖落入本发明的真正精神和范围内的所有这样的修改和变换。The descriptions of the embodiments of the present invention are given above for the understanding of the present invention. It should be understood that the present invention is not limited to the particular embodiments described herein, but that various modifications, rearrangements, and substitutions will now be apparent to those skilled in the art without departing from the scope of the invention. It is therefore intended that the appended claims cover all such modifications and changes as fall within the true spirit and scope of the invention.
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- 2004-08-26 WO PCT/US2004/027740 patent/WO2005020291A2/en active Application Filing
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Also Published As
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| TW200514164A (en) | 2005-04-16 |
| JP2007504652A (en) | 2007-03-01 |
| US7291568B2 (en) | 2007-11-06 |
| US20050048705A1 (en) | 2005-03-03 |
| WO2005020291A2 (en) | 2005-03-03 |
| WO2005020291A3 (en) | 2006-05-18 |
| JP4617306B2 (en) | 2011-01-26 |
| US8709887B2 (en) | 2014-04-29 |
| EP1661163A4 (en) | 2008-08-06 |
| KR20060066069A (en) | 2006-06-15 |
| KR100843496B1 (en) | 2008-07-04 |
| US20080014692A1 (en) | 2008-01-17 |
| EP1661163A2 (en) | 2006-05-31 |
| TWI305383B (en) | 2009-01-11 |
| CN1894781A (en) | 2007-01-10 |
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